scholarly journals Experimental observation of steady inertial wave turbulence in deep rotating flows

2014 ◽  
Vol 10 (7) ◽  
pp. 510-514 ◽  
Author(s):  
Ehud Yarom ◽  
Eran Sharon
2020 ◽  
Vol 125 (25) ◽  
Author(s):  
Eduardo Monsalve ◽  
Maxime Brunet ◽  
Basile Gallet ◽  
Pierre-Philippe Cortet

2018 ◽  
Vol 25 (11) ◽  
pp. 112114 ◽  
Author(s):  
A. D. Patel ◽  
M. Sharma ◽  
R. Ganesh ◽  
N. Ramasubramanian ◽  
P. K. Chattopadhyay

2003 ◽  
Vol 312 (1-2) ◽  
pp. 84-90 ◽  
Author(s):  
J. Pramanik ◽  
B.M. Veeresha ◽  
G. Prasad ◽  
A. Sen ◽  
P.K. Kaw

2004 ◽  
Vol 6 ◽  
pp. 73-73 ◽  
Author(s):  
C Cambon ◽  
R Rubinstein ◽  
F S Godeferd

2019 ◽  
Vol 879 ◽  
pp. 296-326 ◽  
Author(s):  
Thomas Le Reun ◽  
Benjamin Favier ◽  
Michael Le Bars

In this paper, we present an experimental investigation of the turbulent saturation of the flow driven by the parametric resonance of inertial waves in a rotating fluid. In our set-up, a half-metre wide ellipsoid filled with water is brought to solid-body rotation, and then undergoes sustained harmonic modulation of its rotation rate. This triggers the exponential growth of a pair of inertial waves via a mechanism called the libration-driven elliptical instability. Once the saturation of this instability is reached, we observe a turbulent state for which energy is injected into the resonant inertial waves only. Depending on the amplitude of the rotation rate modulation, two different saturation states are observed. At large forcing amplitudes, the saturation flow mainly consists of a steady, geostrophic anticyclone. Its amplitude vanishes as the forcing amplitude is decreased while remaining above the threshold of the elliptical instability. Below this secondary transition, the saturation flow is a superposition of inertial waves which are in weakly nonlinear resonant interaction, a state that could asymptotically lead to inertial wave turbulence. In addition to being a first experimental observation of a wave-dominated saturation in unstable rotating flows, the present study is also an experimental confirmation of the model of Le Reun et al. (Phys. Rev. Lett., vol. 119 (3), 2017, 034502) who introduced the possibility of these two turbulent regimes. The transition between these two regimes and their relevance to geophysical applications are finally discussed.


2006 ◽  
Vol 562 ◽  
pp. 83 ◽  
Author(s):  
F. BELLET ◽  
F. S. GODEFERD ◽  
J. F. SCOTT ◽  
C. CAMBON

1982 ◽  
Vol 120 ◽  
pp. 359-383 ◽  
Author(s):  
E. R. Johnson

The limiting process introduced by Stewartson & Cheng (1979) is used to obtain solutions in the limit of vanishing Rossby number for deep rotating flows at arbitrary Reynolds number over cross-stream ridges of finite slope. Examination of inviscid solutions for infinite-depth flow shows strong dependence on obstacle shape of not only the magnitudes but also the positions of disturbances in the far field. In finite-depth flow there is present the Stewartson & Cheng inertial wave wake, which may be expressed as a sum of vertical modes whose amplitudes depend on the obstacle shape but are independent of distance downstream; the smoother the topography and the shallower the flow, the fewer the number of modes required to describe the motion. For abrupt topography the strength of the wake does not, however, decrease monoton- ically with decreasing container depth (or Rossby number). In very deep flows viscosity causes the wake to decay on a length scale of order the Reynolds number times the ridge width. In shallower flows, where only a few modes are present, the decay of the wake is more rapid. For Reynolds numbers and depths of the order of those in the experiments of Hide, Ibbetson & Lighthill (1968)) viscosity causes the disturbance to take on the appearance of a leaning column.


2005 ◽  
Vol 12 (6) ◽  
pp. 947-953 ◽  
Author(s):  
N. Schaeffer ◽  
P. Cardin

Abstract. We use a quasi-geostrophic numerical model to study the turbulence of rotating flows in a sphere, with realistic Ekman friction and bulk viscous dissipation. The forcing is caused by the destabilization of an axisymmetric Stewartson shear layer, generated by differential rotation, resulting in a forcing at rather large scales. The equilibrium regime is strongly anisotropic and inhomogeneous but exhibits a steep m-5 spectrum in the azimuthal (periodic) direction, at scales smaller than the injection scale. This spectrum has been proposed by Rhines for a Rossby wave turbulence. For some parameter range, we observe a turbulent flow dominated by a large scale vortex located in the shear layer, reminding us of the Great Red Spot of Jupiter.


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